[0001] The present invention relates to a magnetic recording medium and a process for producing
the magnetic recording medium, and more particularly, to a magnetic recording medium
having an excellent surface smoothness without deterioration in coercive force thereof
and a process for producing the magnetic recording medium.
[0002] In recent years, in magnetic recording apparatuses such as a hard disc drive, there
has been a remarkable tendency that information devices or systems used therefor are
miniaturized and required to have a high reliability. With such a recent tendency,
in order to deal with a large capacity data, there is an increasing demand for providing
magnetic recording media on which information can be stored with a high density.
[0003] For satisfying such requirements, the magnetic recording media have been strongly
required to not only have a large coercive force, but also reduce a distance between
a magnetic head and a magnetic recording layer (magnetic spacing).
[0004] As magnetic recording media having a large coercive force, there is widely known
those comprising a substrate and a magnetic thin film formed on the substrate.
[0005] The magnetic thin films which have been already put into practice, are generally
classified into magnetic iron oxide thin films composed of maghemite, etc. (refer
to "Technical Report of Electronic Telecommunication Institute", published by Electronic
Telecommunication Institute, (1981) MR81-20, pp. 5 to 12, "Ceramics", published by
Japan Institute of Ceramics, (1986) Vol. 24, No. 1, pp. 21 to 24, and Japanese Patent
Publication (KOKOKU) Nos. 51-4086(1976) and 5-63925(1993)); and magnetic alloy thin
films composed of Co-Cr alloy; or the like.
[0006] The magnetic iron oxide thin films composed of maghemite are excellent in oxidation
resistance or corrosion resistance due to inherent properties of the oxides. Therefore,
the magnetic iron oxide thin films can show an excellent magnetic stability independent
of change in passage of time and less change in magnetic properties with passage of
time. Further, since oxides exhibit a higher hardness than that of metals, no protective
film is required so that the magnetic spacing of magnetic recording media having such
a magnetic iron oxide thin film can be reduced as compared to that of magnetic recording
media having the magnetic alloy thin film composed of Co-Cr or the like. Therefore,
the magnetic iron oxide thin film is optimum for the production of high-density magnetic
recording media.
[0007] It has been attempted to enhance a coercive force of maghemite thin films by incorporating
cobalt thereinto. However, with the increase in cobalt content, the maghemite thin
films tend to be deteriorated in magnetic stability independent of change in passage
of time due to adverse influences of heat or the like.
[0008] Meanwhile, the present inventors have already proposed a maghemite thin film which
can exhibits a high coercive force even with a less cobalt content by controlling
the specific plane spacing of maghemite crystal (Japanese Patent Application Laid-Open
(KOKAI) Nos. 11-110731(1999) and 11-110732(1999)).
[0009] On the other hand, the magnetic alloy thin films composed of Co-Cr or the like, have
a coercive force as high as not less than about 2,000 Oe. However, these magnetic
alloy thin films are readily oxidized in themselves and, therefore, tend to be deteriorated
in stability independent of change in passage of time as well as magnetic properties.
In order to prevent the deterioration of magnetic properties due to the oxidation,
a protective film of diamond-like carbon, SiO
2 or the like having a thickness of usually 100 to 200 Å, is formed on the surface
of the magnetic alloy thin film, thereby causing the increase in magnetic spacing
corresponding to the thickness of the protective film.
[0010] In magnetic recording media, in order to reduce the magnetic spacing, it is necessary
to reduce the fly-heights of magnetic head and always cause the magnetic head to be
flying stably. In conventional hard disc drive devices, magnetic recording media used
therefor have been required to have some surface roughness in order to prevent the
magnetic head from being absorbed onto the magnetic recording medium surface due to
a meniscus force upon landing on the surface thereof. At the present time, due to
the improvement in hard disc systems, magnetic recording media have been no longer
required to show such a surface roughness for preventing the magnetic head from being
absorbed thereonto. Rather, it has been required that magnetic thin films used in
these magnetic recording media have a more excellent surface smoothness.
[0011] Also, it is known that the non-smooth surface of magnetic recording media causes
media noise. In order to eliminate such a media noise, it is necessary to lessen a
surface roughness of the magnetic thin film.
[0012] At present, in magnetic recording media having a magnetic oxide thin film, the surface
property of the magnetic thin film largely depends on that of an underlying substrate
due to its extremely small thickness such as not more than 50 nm. Therefore, it has
been required not only to use such a substrate having an excellent surface smoothness,
but also to develop techniques for further smoothening the surface of magnetic thin
film.
[0013] Hitherto, as processes of producing maghemite thin films, there are known (1) a process
comprising forming a hematite thin film on a substrate, reducing the hematite thin
film at a temperature of 230 to 320°C to transform the hematite thin film into a magnetite
thin film, and then oxidizing the magnetite thin film at a temperature of 290 to 330°C;
(2) a process comprising forming a magnetite thin film on a substrate and oxidizing
the magnetite thin film at a temperature of not less than 320°C; or the like.
[0014] Also, as techniques for improving the surface smoothness of magnetic recording media
having a magnetic iron oxide thin film, there are known a process of enhancing the
surface smoothness under optimized heat-treatment conditions (Japanese Patent No.
2,816,472); a process of sputter-etching the surface of a magnetic recording layer
composed of a metal thin film using an oxygen gas (Japanese Patent Application Laid-Open
(KOKAI) No. 10-50544(1998)); or the like.
[0015] Presently, it has been strongly demanded to provide magnetic recording media having
a maghemite thin film capable of showing an excellent surface smoothness while maintaining
as much as possible a high coercive force thereof. However, such magnetic recording
media satisfying these requirements have not been obtained until now.
[0016] Namely, in the process described in Japanese Patent No. 2,816,472, the surface roughness
of the glass substrate is reduced by polishing or the like, and the oxidation of the
magnetite thin film is conducted in an atmospheric air by appropriately selecting
conditions therefor, thereby obtaining magnetic recording media having a low maximum
height (R
max). However, since the thickness of the magnetic thin film is 200 nm in Example of
Japanese Patent No. 2,816,472, in the case where the thickness of the magnetic thin
film is extremely small, e.g., as small as not more than 50 nm, it is hard to say
that the surface roughness of magnetic recording media can be sufficiently improved
maintaining as much as possible a high coercive force thereof.
[0017] Also, the process described in Japanese Patent Application Laid-Open (KOKAI) No.
10-50544(1998) is directed to the technique for improving the surface smoothness of
magnetic recording media having an alloy thin film containing cobalt as a main component.
However, in this process, it is required to subject the final product to plasma treatment.
Meanwhile, if the maghemite thin film used in the present invention is subjected to
the similar plasma treatment, the maghemite thin film suffers from local discoloration,
thereby failing to obtain the aimed effect.
[0018] As a result of the present inventors' earnest studies for solving the above problems,
it has been found that in the process for producing a magnetic recording medium wherein
a magnetite thin film is formed on a substrate and then the magnetite thin film is
oxidized to a maghemite thin film, by subjecting the magnetite thin film before oxidized
to plasma treatment using an oxygen gas or an oxygen-containing mixed gas, the surface
of the obtained maghemite thin film formed on the substrate exhibits a center line
average roughness (= an average roughness)(Ra) of 0.1 to 0.7 nm and a maximum height
(= a max height) (R
max) of 1 to 10 nm. The present invention has been attained based on the finding.
[0019] It is an object of the present invention to provide a magnetic recording medium which
can exhibit an excellent surface smoothness without deterioration in high coercive
force thereof.
[0020] It is another object of the present invention to provide a economically useful process
for producing a maghemite thin film capable of enhancing a surface smoothness of a
magnetic layer without deterioration in its high coercive force thereof.
[0021] In a first aspect of the present invention, there is provided a magnetic recording
medium comprising a substrate and a maghemite thin film formed on the substrate, which
maghemite thin film has a thickness of 10 to 50 nm and a surface roughness represented
by an average roughness (Ra) of 0.1 to 0.7 nm and a max height (R
max) of 1 to 10 nm.
[0022] In a second aspect of the present invention, there is provided a magnetic recording
medium comprising a substrate, a nickel oxide thin film formed on the substrate and
a maghemite thin film formed on the nickel oxide thin film, which maghemite thin film
has a thickness of 10 to 50 nm and a surface roughness represented by an average roughness
(Ra) of 0.1 to 0.7 nm and a max height (R
max) of 1 to 10 nm.
[0023] In a third aspect of the present invention, there is provided a process for producing
a magnetic recording medium, comprising the steps of forming a magnetite thin film
on a substrate; subjecting the magnetite thin film to plasma treatment using an oxygen
gas or an oxygen-containing mixed gas; and oxidizing the thus treated magnetite thin
film into a maghemite thin film.
[0024] Fig. 1 is a diagram showing X-ray diffraction patterns (a) and (b) of a magnetite
thin film before and after plasma treatment, respectively, according to the present
invention.
[0025] The present invention will be described in detail below.
[0026] First, the magnetic recording medium of the present invention is described.
[0027] The magnetic recording medium of the present invention comprises:
(I) a substrate and a maghemite thin film formed on the substrate; or
(II) a substrate, a nickel oxide thin film formed on the substrate and a maghemite
thin film formed on the nickel oxide thin film.
[0028] As the substrate used in the present invention, there may be exemplified substrates
generally used for this purpose, such as plastic substrates, glass substrates or the
like. Among these substrates, the glass substrates are preferred. The surface of the
substrate used in the present invention, has the average roughness (Ra) of usually
not more than 0.6 nm, preferably 0.1 to 0.5 nm; and the max height (R
max) of usually not more than 8 nm, preferably 1 to 7 nm.
[0029] The maghemite thin film used in the present invention has a thickness of usually
10 to 50 nm, preferably 10 to 30 nm, more preferably 10 to 20 nm. When the thickness
of the maghemite thin film is less than 10 nm, it may be difficult to obtain a magnetic
recording medium having a coercive force of not less than 2,000 Oe. When the thickness
of the maghemite thin film is more than 50 nm, it may become difficult to uniformly
magnetize the maghemite thin film up to a deep portion thereof when signals are recorded
thereon, thereby failing to achieve good recording and reproducing characteristics.
[0030] Maghemite is generally represented by the general formula: γ-Fe
2O
3. However, the maghemite used in present invention may contain a small amount of Fe
2+.
[0031] The maghemite thin film used in the present invention may contain cobalt in a predetermined
amount for enhancing a coercive force thereof. The amount of cobalt incorporated in
the maghemite thin film is adjusted such that the molar ratio of Co to Fe is in the
range of usually not more than 0.2:1, preferably 0.01:1 to 0.1:1. When the content
of cobalt is less than 0.01:1, it may tend to be difficult to obtain a magnetic recording
medium having a coercive force as high as not less than 2,000 Oe. When the content
of cobalt is more than 0.2:1, it may tend to be difficult to obtain a magnetic recording
medium having an excellent magnetic stability independent of change in passage of
time.
[0032] Meanwhile, the maghemite thin film of the present invention may contain, if required,
any of elements other than cobalt which are ordinarily used to improve various properties
thereof, such as Mn, Ni, Cu, Ti, Zn or the like, at a molar ratio of the element to
Fe of usually not more than 0.04:1, preferably 0.005:1 to 0.04:1. In this case, the
addition of these elements facilitates the production of magnetic recording media
having a high coercive force as well as the incorporation of cobalt.
[0033] Among various surface roughness parameters of the maghemite thin film, the average
roughness (Ra) thereof is usually 0.1 to 0.7 nm, preferably 0.1 to 0.65 nm, more preferably
0.1 to 0.62 nm. When the average roughness (Ra) is more than 0.7 nm, it is not possible
to obtain the aimed effect of the present invention.
[0034] Among the surface roughness parameters of the maghemite thin film, the max height
(R
max thereof is usually 1 to 10 nm, preferably 1 to 9.5 nm. When the max height (R
max) is more than 10 nm, it may difficult to obtain the aimed effect of the present invention.
[0035] The magnetic recording medium of the present invention has a saturation magnetization
value (value of magnetization when applying a magnetic field of 20 KOe thereto) of
usually 220 to 300 emu/cm
3, preferably 230 to 280 emu/cm
3, more preferably 230 to 260 emu/cm
3; and a coercive force value of usually not less than 1,800 Oe, preferably not less
than 1,900 Oe. The upper limit of the coercive force value is preferably 4,000 Oe.
[0036] The magnetic recording medium having the maghemite thin film containing cobalt of
the present invention has a coercive force value of usually not less than 2,000 Oe,
preferably not less than 2,200 Oe, more preferably not less than 3,000 Oe. The upper
limit of the coercive force value is preferably 4,000 Oe.
[0037] In the magnetic recording medium of the present invention, a nickel oxide thin film
as an underlaying film may be disposed between the substrate and the maghemite thin
film. When the nickel oxide thin film is formed as an underlaying film for the maghemite
thin film, the obtained magnetic recording medium not only can be improved in magnetic
properties, especially coercive force, but also have a high coercive force even if
the thickness of the maghemite thin film is thinner as compared with the that of the
magnetic recording medium having no underlaying film. Further the surface smoothness
of the maghemite thin film can be improved by thinning the thickness of the maghemite
thin film. The thickness of the nickel oxide thin film is usually 50 to 100 nm.
[0038] In the case of the magnetic recording medium having the nickel oxide thin film sandwiched
between the substrate and the maghemite thin film, the average roughness (Ra) thereof
is usually 0.1 to 0.7 nm, preferably 0.1 to 0.65 nm, more preferably 0.1 to 0.6 nm,
still more preferably 0.1 to 0.56 nm. When the average roughness (Ra) is more than
0.7 nm, it may be difficult to obtain the aimed effect of the present invention.
[0039] In the case of the magnetic recording medium having the nickel oxide thin film sandwiched
between the substrate and the maghemite thin film, the max height (R
max) thereof is usually 1 to 10 nm, preferably 1 to 9 nm, more preferably 1 to 8 nm,
still more preferably 1 to 7.5 nm. When the max height (R
max) is more than 10 nm, it may be difficult to obtain the aimed effect of the present
invention.
[0040] The magnetic recording medium having the nickel oxide thin film sandwiched between
the substrate and the maghemite thin film, has a saturation magnetization value (value
of magnetization when applying a magnetic field of 20 KOe thereto) of usually 220
to 300 emu/cm
3, preferably 230 to 280 emu/cm
3, more preferably 230 to 260 emu/cm
3; and a coercive force value of usually not less than 2,000 Oe, preferably not less
than 2,200 Oe, more preferably not less than 2,800 Oe. The upper limit of the coercive
force value is preferably 8,000 Oe.
[0041] The magnetic recording medium having the nickel oxide thin film sandwiched between
the substrate and the maghemite thin film containing cobalt, has a coercive force
value of usually not less than 2,200 Oe, preferably not less than 2,500 Oe, more preferably
not less than 3,200 Oe. The upper limit of the coercive force value is preferably
8,000 Oe.
[0042] Next, the process for producing the magnetic recording medium according to the present
invention is described.
[0043] The magnetic recording medium of the present invention can be produced by subjecting
a magnetite thin film formed on a substrate to plasma treatment using an oxygen gas
or an oxygen-containing mixed gas, and then oxidizing the magnetite thin film at a
temperature of 200 to 450°C to transform the magnetite thin film into a maghemite
thin film.
[0044] The magnetite thin film can be formed on the substrate by an ordinary method. For
example, the magnetite thin film may be formed on the substrate by a so-called sputtering
method, i.e., by producing and depositing magnetite using an Fe alloy target in the
presence of an introduced mixed gas of oxygen and noble gas, while appropriately controlling
the oxygen flow rate (CCM) in the mixed gas and the magnetite deposition rate (nm/min.).
[0045] The oxygen flow rate (CCM) in the mixed gas relative to the magnetite deposition
rate (nm/min.) may vary depending upon various conditions for obtaining the magnetite
thin film by oxidizing the Fe alloy target, for example, kind and structure of apparatus
used, total gas pressure, substrate temperature, area of sputtering target or the
like.
[0046] The magnetite thin film prior to being subjected to the plasma treatment, has a thickness
of usually 10 to 50 nm, and a surface roughness represented by the average roughness
(Ra) of usually 0.1 to 0.7 nm and the max height (R
max) of usually 1 to 10 nm.
[0047] The plasma treatment of the magnetite thin film according to the present invention
may be conducted at a substrate temperature of usually 100 to 220°C, preferably 150
to 220°C. When the substrate temperature is out of the above specified range, a sufficient
effect may not be obtained.
[0048] The plasma treatment of the magnetite thin film may be conducted in an atmosphere
containing an oxygen gas or an oxygen-containing mixed gas.
[0049] As the oxygen-containing mixed gas, there may be preferably used a mixed gas composed
of an oxygen gas and a noble gas. Examples of the noble gases may include helium,
neon, argon, krypton, xenon, radon or the like. Among these noble gases, argon is
preferred in the consideration of economy, the mixing ratio of the oxygen gas to the
noble gas in the mixed gas is usually 100:0 to 50:50.
[0050] The plasma-treating time in the present invention is usually 30 seconds to 30 minutes,
preferably 1.5 to 30 minutes. When the plasma-treating time is out of the above specified
range, a sufficient effect may not be obtained.
[0051] The magnetite thin film after the plasma treatment, has a thickness of usually 10
to 50 nm, and a surface roughness represented by the average roughness (Ra) of usually
0.1 to 0.7 nm and the max height (R
max) of 1 to 10 nm.
[0052] In the case where the nickel oxide thin film is used as the underlaying film, the
nickel oxide thin film is preliminarily formed on the substrate, and then the magnetite
thin film is formed thereon by the same method as described above.
[0053] The most important point of the present invention lies in the fact that by subjecting
the magnetite thin film before the oxidation treatment, to plasma treatment in an
atmosphere containing an oxygen gas or an oxygen-containing mixed gas, the obtained
maghemite thin film as a final product can be improved in surface smoothness.
[0054] The reason why the surface smoothness of the maghemite thin film can be enhanced,
is considered as follows, though not exactly known. That is, by subjecting the magnetite
thin film before the oxidation treatment, to plasma treatment in an atmosphere containing
an oxygen gas or an oxygen-containing mixed gas, the oxidation of an insufficiently
oxidized portion in the magnetite thin film can be promoted, thereby obtaining a more
homogeneous magnetite thin film. Then, when such a uniformly oxidized magnetite thin
film is subjected to an oxidation treatment, the thin film can be more uniformly oxidized
and, as a result, transformed into a maghemite thin film having an excellent surface
smoothness.
[0055] Meanwhile, in the case where the magnetite thin film is directly oxidized without
conducting the plasma treatment, since the magnetite thin film to be subjected to
the oxidation treatment, still contains an insufficiently oxidized portion therein,
it is not possible to obtain a maghemite thin film having a sufficient surface smoothness.
That is, the obtained maghemite thin film has the average roughness (Ra) of more than
0.7 nm and the max height (R
max) of more than 10 nm.
[0056] As shown in Fig. 1, from the comparison between X-ray diffraction patterns of the
magnetite thin film before and after the plasma treatment, it is recognized that the
plane (311) of the magnetite after the plasma treatment ("b" in Fig. 1) has been shifted
to a high angle side as compared to that of the magnetite prior to the plasma treatment
("a" in Fig. 1). This indicates that the spacing of the plane (311) of the magnetite
has been narrowed by the plasma treatment, thereby causing a structural change thereof.
In general, it is known that when magnetite is transformed into maghemite having a
higher degree of oxidation, the plane (311) is narrowed.
[0057] Thus, the above fact also shows that the oxidation of the magnetite thin film can
be promoted by the plasma treatment.
[0058] The magnetic recording medium of the present invention can exhibit an excellent surface
smoothness without deterioration in high coercive force thereof and, therefore, is
suitable as those for high-density recording.
EXAMPLES
[0059] The present invention is described in more detail by Examples and Comparative Examples,
but the Examples are only illustrative and, therefore, not intended to limit the scope
of the present invention.
[0060] Various properties were measured by the following methods.
(1) The surface roughness (average roughness (Ra) and max height (Rmax)) of the magnetite thin film or maghemite thin film is measured using an atomic force
microscope (manufactured by Digital Instruments (D.I.)), and evaluated with respect
to a 5 µm-square area of each film.
(2) The thickness of a magnetic recording layer of the magnetite thin film or maghemite thin film is determined as follows. That
is, before the formation of the thin film, a line is drawn on a substrate using a
felt pen. Then, after the formation of the thin film on the substrate, a part of the
formed film and the underlying drawn line are simultaneously removed using an organic
solvent. The thus formed stepped portion is measured by a tracer-type surface roughness
tester (manufactured by DEKTAK). The thickness of the thin film is calculated from
the measured value.
(3) The oxidation of the magnetite thin film into the maghemite thin film is confirmed by the change
in surface resistivity of the thin film as an index of the oxidation thereof.
That is, the surface resistivity of the magnetite thin film is in the range of 0.001
to 0.5 MΩ, whereas the surface resistivity of the maghemite thin film is raised from
1 to 100 MΩ and varied over the range. The surface resistivity is measured by an Insulation
Tester DM-1527 (manufactured by Sanwa Denki Keiki Co., Ltd.) by setting the distance
between two probes to 10 mm.
(4) The magnetic propertiei such as coercive force and saturation magnetization of the magnetic recording medium,
are expressed by the values measured using "Vibrating Sample Magnetometer VSM" (manufactured
by TOEI KOGYO CO., LTD.) by applying a magnetic field of 20 KOe in maximum thereto.
(5) The X-ray diffraction patterns of the respective thin films are expressed by values measured by "X-Ray Diffractometer
RAD-IIA" (manufactured by RIGAKU DENKI CO., LTD.).
[0061] The measuring conditions of the X-ray diffraction patterns are as follow:
Lamp used: Fe; lamp voltage: 40 kV; lamp current: 25 mA; sampling width of goniometer:
0.010°; scanning speed: 1.000°/min.; light-emitting (divergent) slit: 1°; scattering
slit: 1°; light-receiving slit: 0.30 mm.
[0062] The region covering a diffraction angle (2θ) of 30.00° to 60.00° is measured under
the above-mentioned conditions.
Example 1:
<Production of magnetic recording medium>
[0063] The process for producing a magnetic recording medium by directly forming a magnetite
thin film on a substrate is described below.
[0064] Using an RF sputtering apparatus (High Rate Sputtering Apparatus "SH-250H-T06" manufactured
by NIHON SHINKU CO., LTD.), a magnetite thin film containing cobalt was formed on
a crystallized glass substrate having the average roughness (Ra) of 0.20 nm and the
max height (R
max) of 5.00 nm, by a reactive sputtering method (substrate temperature: 220°C; gas pressure:
9 mTorr) using an Fe alloy target containing cobalt (Co content: 4 % by weight). The
thus obtained magnetite thin film containing cobalt had the thickness of 48 nm, the
average roughness (Ra) of 0.57 nm and the max height (R
max) of 8.00 nm.
[0065] Next, an oxygen gas was introduced into the RF sputtering apparatus to produce a
plasma in an etching mode. The thus produced plasma was irradiated on the magnetite
thin film for 30 minutes (substrate temperature: 180°C; gas pressure: 9 mTorr; making
power: 100 W).
[0066] After the plasma treatment, the magnetite thin film containing cobalt showed the
average roughness (Ra) of 0.62 nm and the max height (R
max of 8.12 nm.
[0067] Successively, the magnetite thin film containing cobalt was oxidized at 320°C for
60 minutes in an atmospheric air, thereby obtaining a maghemite thin film containing
cobalt (Co:Fe (mole ratio) = 0.04:1).
[0068] The thus obtained maghemite thin film containing cobalt had the thickness of 48 nm,
a surface roughness represented by the average roughness (Ra) of 0.64 nm, the max
height (R
max) of 8.72 nm, the saturation magnetization value of 244 emu/cm
3, and the coercive force of 3,080 Oe.
[0069] For your reference, the maghemite thin film containing cobalt produced without the
plasma treatment showed a surface roughness represented by the average roughness (Ra)
of 0.88 nm and the max height (R
max) of 14.7 nm, the saturation magnetization value of 255 emu/cm
3 and the coercive force of 3,001 Oe.
[0070] As seen from the above, it was confirmed that by subjecting the magnetite thin film
prior to the oxidation to the plasma treatment, the surface smoothness of the obtained
maghemite thin film could be enhanced maintaining as much as possible a high coercive
force.
Examples 2 to 6 and Comparative Examples 1 to 3:
[0071] The same procedure as defined in Example 1 was conducted except that a kind of the
target and the plasma treatment conditions for the magnetite thin film were changed
variously, thereby obtaining a maghemite thin film.
[0072] The production conditions are shown in Table 1 and various properties of the obtained
maghemite thin film are shown in Table 2.
Examples 7 to 14 and Comparative Examples 4 to 6:
[0073] The same procedure as defined in Example 1 was conducted except that a nickel oxide
thin film having a thickness of 100 nm was first formed on the glass substrate and
then the magnetite thin film was formed thereon, and the plasma treatment conditions
for the magnetite thin film were changed variously, thereby obtaining a maghemite
thin film.
[0074] The production conditions are shown in Table 3 and various properties of the obtained
maghemite thin film are shown in Table 4.